S. Blessing
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Research Interests
S. Blessing has a total of 1000 co-authors. Here are the top co-authors by number of shared publications:
- Horst D. Wahl
Florida State University, Tallahassee, Florida 32306, USA
447 shared publications - David Hedin
Northern Illinois University, DeKalb, Illinois 60115, USA
446 shared publications - Gerald Blazey
Northern Illinois University
446 shared publications - P. D. Grannis
State University of New York, Stony Brook, New York 11794, USA
446 shared publications - A. P. Heinson
University of California Riverside, Riverside, California 92521, USA
445 shared publications - Bruce Hoeneisen
Universidad San Francisco de Quito Quito Ecuador
443 shared publications
Latest Publications
- Open Access
- 8 December 2014
- Published by American Physical Society (APS) in Physical Review D
- Vol. 90 (11) , 111101
Observation and studies of doubleproduction at the TevatronWe present the observation of doubly produced mesons with the D0 detector at Fermilab in collisions at . The production cross section for both singly and doubly produced mesons is measured using a sample with an integrated luminosity of . For the first time, the double production cross section is separated into contributions due to single and double parton scatterings. Using these measurements, we determine the effective cross section , a parameter characterizing an effective spatial area of the parton-parton interactions and related to the parton spatial density inside the nucleon.- 8 December 2014
- Published by American Physical Society (APS) in Physical Review D
- Vol. 90 (11) , 111101
Open AccessObservation and studies of doubleproduction at the TevatronWe present the observation of doubly produced mesons with the D0 detector at Fermilab in collisions at . The production cross section for both singly and doubly produced mesons is measured using a sample with an integrated luminosity of . For the first time, the double production cross section is separated into contributions due to single and double parton scatterings. Using these measurements, we determine the effective cross section , a parameter characterizing an effective spatial area of the parton-parton interactions and related to the parton spatial density inside the nucleon. - 1 December 2014
- Published by Office of Scientific and Technical Information (OSTI)
FSU High Energy Physics
The High Energy Physics group at Florida State University (FSU), which was established in 1958, is engaged in the study of the fundamental constituents of matter and the laws by which they interact. The group comprises theoretical and experimental physicists, who sometimes collaborate on projects of mutual interest. The report highlights the main recent achievements of the group. Significant, recent, achievements of the group’s theoretical physicists include progress in making precise predictions in the theory of the Higgs boson and its associated processes, and in the theoretical understanding of mathematical quantities called parton distribution functions that are related to the structure of composite particles such as the proton. These functions are needed to compare data from particle collisions, such as the proton-proton collisions at the CERN Large Hadron Collider (LHC), with theoretical predictions. The report also describes the progress in providing analogous functions for heavy nuclei, which find application in neutrino physics. The report highlights progress in understanding quantum field theory on a lattice of points in space and time (an area of study called lattice field theory), the progress in constructing several theories of potential new physics that can be tested at the LHC, and interesting new ideas inmore » the theory of the inflationary expansion of the very early universe. The focus of the experimental physicists is the Compact Muon Solenoid (CMS) experiment at CERN. The report, however, also includes results from the D0 experiment at Fermilab to which the group made numerous contributions over a period of many years. The experimental group is particularly interested in looking for new physics at the LHC that may provide the necessary insight to extend the standard model (SM) of particle physics. Indeed, the search for new physics is the primary task of contemporary particle physics, one motivated by the need to explain certain facts, such as the non-zero neutrino masses or the overwhelming astrophysical evidence for an invisible form of matter, called dark matter, that has had a marked effect on the evolution of structure in the universe. The report highlights the main, recent, experimental achievements of the experimental group, which include the investigation of properties of the W and Z bosons; the search for new heavy stable charged particles and the search for a proposed property of nature called supersymmetry in proton-proton collisions that yield high energy photons. In addition, we report a few results from a more general search for supersymmetry at the LHC, initiated by the group. The report also highlights the group's significant contributions, both theoretical and experimental, to the 2012 discovery of the Higgs boson and the measurement of its properties.« less
- 1 December 2014
- Published by Office of Scientific and Technical Information (OSTI)
FSU High Energy Physics
The High Energy Physics group at Florida State University (FSU), which was established in 1958, is engaged in the study of the fundamental constituents of matter and the laws by which they interact. The group comprises theoretical and experimental physicists, who sometimes collaborate on projects of mutual interest. The report highlights the main recent achievements of the group. Significant, recent, achievements of the group’s theoretical physicists include progress in making precise predictions in the theory of the Higgs boson and its associated processes, and in the theoretical understanding of mathematical quantities called parton distribution functions that are related to the structure of composite particles such as the proton. These functions are needed to compare data from particle collisions, such as the proton-proton collisions at the CERN Large Hadron Collider (LHC), with theoretical predictions. The report also describes the progress in providing analogous functions for heavy nuclei, which find application in neutrino physics. The report highlights progress in understanding quantum field theory on a lattice of points in space and time (an area of study called lattice field theory), the progress in constructing several theories of potential new physics that can be tested at the LHC, and interesting new ideas inmore » the theory of the inflationary expansion of the very early universe. The focus of the experimental physicists is the Compact Muon Solenoid (CMS) experiment at CERN. The report, however, also includes results from the D0 experiment at Fermilab to which the group made numerous contributions over a period of many years. The experimental group is particularly interested in looking for new physics at the LHC that may provide the necessary insight to extend the standard model (SM) of particle physics. Indeed, the search for new physics is the primary task of contemporary particle physics, one motivated by the need to explain certain facts, such as the non-zero neutrino masses or the overwhelming astrophysical evidence for an invisible form of matter, called dark matter, that has had a marked effect on the evolution of structure in the universe. The report highlights the main, recent, experimental achievements of the experimental group, which include the investigation of properties of the W and Z bosons; the search for new heavy stable charged particles and the search for a proposed property of nature called supersymmetry in proton-proton collisions that yield high energy photons. In addition, we report a few results from a more general search for supersymmetry at the LHC, initiated by the group. The report also highlights the group's significant contributions, both theoretical and experimental, to the 2012 discovery of the Higgs boson and the measurement of its properties.« less
- Open Access
- 19 November 2014
- Published by American Physical Society (APS) in Physical Review D
- Vol. 90 (9) , 092006
Measurement of differentialproduction cross sections incollisionsThe production of top quark-antiquark pair events in collisions at is studied as a function of the transverse momentum and absolute value of the rapidity of the top quarks as well as of the invariant mass of the pair. We select events containing an isolated lepton, a large imbalance in transverse momentum, and four or more jets with at least one jet identified as originating from a quark. The data sample corresponds to of integrated luminosity recorded with the D0 detector during Run II of the Fermilab Tevatron Collider. Observed differential cross sections are consistent with standard model predictions.- 19 November 2014
- Published by American Physical Society (APS) in Physical Review D
- Vol. 90 (9) , 092006
Open AccessMeasurement of differentialproduction cross sections incollisionsThe production of top quark-antiquark pair events in collisions at is studied as a function of the transverse momentum and absolute value of the rapidity of the top quarks as well as of the invariant mass of the pair. We select events containing an isolated lepton, a large imbalance in transverse momentum, and four or more jets with at least one jet identified as originating from a quark. The data sample corresponds to of integrated luminosity recorded with the D0 detector during Run II of the Fermilab Tevatron Collider. Observed differential cross sections are consistent with standard model predictions. - 1 November 2014
- Published by Elsevier in Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
- Vol. 763, 290-303
Improved b quark jet identification at the D0 experiment
- 1 November 2014
- Published by Elsevier in Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
- Vol. 763, 290-303
Improved b quark jet identification at the D0 experiment
- 29 October 2014
- Published by American Physical Society (APS) in Physical Review D
- Vol. 90 (7) , 072011
Measurement of the forward-backward asymmetry in top quark-antiquark production incollisions using thechannelWe present a measurement of the forward–backward asymmetry in top quark–antiquark production using the full Tevatron Run II data set collected by the D0 experiment at Fermilab. The measurement is performed in final states using a new kinematic fitting algorithm for events with four or more jets and a new partial reconstruction algorithm for events with only three jets. Corrected for detector acceptance and resolution effects, the asymmetry is evaluated to be . Results are consistent with the standard model predictions which range from 5.0% to 8.8%. We also present the dependence of the asymmetry on the invariant mass of the top quark–antiquark system and the difference in rapidities of the top quark and antiquark.- 29 October 2014
- Published by American Physical Society (APS) in Physical Review D
- Vol. 90 (7) , 072011
Measurement of the forward-backward asymmetry in top quark-antiquark production incollisions using thechannelWe present a measurement of the forward–backward asymmetry in top quark–antiquark production using the full Tevatron Run II data set collected by the D0 experiment at Fermilab. The measurement is performed in final states using a new kinematic fitting algorithm for events with four or more jets and a new partial reconstruction algorithm for events with only three jets. Corrected for detector acceptance and resolution effects, the asymmetry is evaluated to be . Results are consistent with the standard model predictions which range from 5.0% to 8.8%. We also present the dependence of the asymmetry on the invariant mass of the top quark–antiquark system and the difference in rapidities of the top quark and antiquark.- Open Access
- 7 October 2014
- Published by American Physical Society (APS) in Physical Review D
- Vol. 90 (7) , 072001
Measurement of the forward-backward asymmetry in the distribution of leptons inevents in thechannelWe present measurements of the forward-backward asymmetry in the angular distribution of leptons from decays of top quarks and antiquarks produced in proton-antiproton collisions. We consider the final state containing a lepton and at least three jets. The entire sample of data collected by the D0 experiment during Run II of the Fermilab Tevatron Collider, corresponding to of integrated luminosity, is used. The asymmetry measured for reconstructed leptons is . When corrected for efficiency and resolution effects within the lepton rapidity coverage of , the asymmetry is found to be . We examine the dependence of on the transverse momentum and rapidity of the lepton. Combination with the asymmetry measured in the final states containing two leptons yields . The results are in agreement with predictions from the next-to-leading-order QCD generator mc@nlo, which predicts an asymmetry of for .- 7 October 2014
- Published by American Physical Society (APS) in Physical Review D
- Vol. 90 (7) , 072001
Open AccessMeasurement of the forward-backward asymmetry in the distribution of leptons inevents in thechannelWe present measurements of the forward-backward asymmetry in the angular distribution of leptons from decays of top quarks and antiquarks produced in proton-antiproton collisions. We consider the final state containing a lepton and at least three jets. The entire sample of data collected by the D0 experiment during Run II of the Fermilab Tevatron Collider, corresponding to of integrated luminosity, is used. The asymmetry measured for reconstructed leptons is . When corrected for efficiency and resolution effects within the lepton rapidity coverage of , the asymmetry is found to be . We examine the dependence of on the transverse momentum and rapidity of the lepton. Combination with the asymmetry measured in the final states containing two leptons yields . The results are in agreement with predictions from the next-to-leading-order QCD generator mc@nlo, which predicts an asymmetry of for . - Open Access
- 8 September 2014
- Published by Elsevier in Physics Letters B
- Vol. 737, 357-365
Measurement of the differential γ+2b-jet cross section and the ratio σ(γ+2b-jets)/σ(γ+b-jet) in pp¯ collisions at s=1.96TeV
- 8 September 2014
- Published by Elsevier in Physics Letters B
- Vol. 737, 357-365
Open AccessMeasurement of the differential γ+2b-jet cross section and the ratio σ(γ+2b-jets)/σ(γ+b-jet) in pp¯ collisions at s=1.96TeV
- Open Access
- 17 July 2014
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 113 (3) , 032002
Precision Measurement of the Top Quark Mass in Lepton+Jets Final States
We measure the mass of the top quark in final states using the full sample of collision data collected by the D0 experiment in Run II of the Fermilab Tevatron Collider at , corresponding to of integrated luminosity. We use a matrix element technique that calculates the probabilities for each event to result from production or background. The overall jet energy scale is constrained in situ by the mass of the boson. We measure . This constitutes the most precise single measurement of the top-quark mass.- 17 July 2014
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 113 (3) , 032002
Open AccessPrecision Measurement of the Top Quark Mass in Lepton+Jets Final States
We measure the mass of the top quark in final states using the full sample of collision data collected by the D0 experiment in Run II of the Fermilab Tevatron Collider at , corresponding to of integrated luminosity. We use a matrix element technique that calculates the probabilities for each event to result from production or background. The overall jet energy scale is constrained in situ by the mass of the boson. We measure . This constitutes the most precise single measurement of the top-quark mass. - 26 June 2014
- Published by Elsevier in Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
- Vol. 763, 442-475
Jet energy scale determination in the D0 experiment
- 26 June 2014
- Published by Elsevier in Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
- Vol. 763, 442-475
Jet energy scale determination in the D0 experiment
- Open Access
- 9 June 2014
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 112 (23) , 231803
Observation of-Channel Production of Single Top Quarks at the TevatronWe report the first observation of single-top-quark production in the channel through the combination of the CDF and D0 measurements of the cross section in proton-antiproton collisions at a center-of-mass energy of 1.96 TeV. The data correspond to total integrated luminosities of up to per experiment. The measured cross section is . The probability of observing a statistical fluctuation of the background to a cross section of the observed size or larger is , corresponding to a significance of 6.3 standard deviations for the presence of an -channel contribution to the production of single-top quarks.- 9 June 2014
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 112 (23) , 231803
Open AccessObservation of-Channel Production of Single Top Quarks at the TevatronWe report the first observation of single-top-quark production in the channel through the combination of the CDF and D0 measurements of the cross section in proton-antiproton collisions at a center-of-mass energy of 1.96 TeV. The data correspond to total integrated luminosities of up to per experiment. The measured cross section is . The probability of observing a statistical fluctuation of the background to a cross section of the observed size or larger is , corresponding to a significance of 6.3 standard deviations for the presence of an -channel contribution to the production of single-top quarks.